Abstract
The general theory of thermal ignition under the conditions of thermal analysis of flammable substances is discussed. For a linear heating rate of the specimen the ignition temperature is obtained from the relationship $$(dT/dt)_b - \frac{q}{{(dT/dt)_b }} = \frac{E}{{RT_b^2 }}(T_b - T_c^\prime )$$ whereT′c is the temperature of the reactor wall (heated at the rateq) at the starting moment of the development of the thermal explosion.
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